{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:UK52663MQH6DLNDCTK65RDVQV5","short_pith_number":"pith:UK52663M","schema_version":"1.0","canonical_sha256":"a2bbaf7b6c81fc35b4629abdd88eb0af5f9a24f5353682ba0f1ab5643c665094","source":{"kind":"arxiv","id":"hep-ph/9303282","version":2},"attestation_state":"computed","paper":{"title":"First Order Phase Transition in a Two Higgs-doublet Model with $M_{h}>M_{W}$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aris Papadopoulos, Vidyut Jain","submitted_at":"1993-03-18T23:27:04Z","abstract_excerpt":"We study the 3d effective field theory of a weakly coupled two Higgs-doublet scalar model at high temperature. Our model has three scalar quartic couplings and an $O(4)$ symmetry which is spontaneously broken by a nonzero scalar field $vev$ at zero temperature. Using high temperature perturbation theory, renormalization group arguments in $4-\\epsilon$ dimensions, as well as $1/N$ expansion techniques in 3 dimensions, we argue that the transition from the high temperature symmetry restoring phase to the low temperature phase is first order for a range of scalar couplings. This result is not due"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/9303282","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1993-03-18T23:27:04Z","cross_cats_sorted":[],"title_canon_sha256":"1d9cc38f25eee5f0779831200a1fce72a7710f0230ad2179747e26648874d333","abstract_canon_sha256":"de0f6c764e53fdc3dce950803516270932dbf1e1294a7ac93561f7e9508d4c61"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:37:55.502086Z","signature_b64":"+p6CLYu6/d90HJQdyPGQWXbR2LoSCU3Yd86SvkcxpKAgGVL9GFDh1XkaM7iajkpp/PDfZCsgTCr6m+79JTFJBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a2bbaf7b6c81fc35b4629abdd88eb0af5f9a24f5353682ba0f1ab5643c665094","last_reissued_at":"2026-05-18T04:37:55.501300Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:37:55.501300Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"First Order Phase Transition in a Two Higgs-doublet Model with $M_{h}>M_{W}$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aris Papadopoulos, Vidyut Jain","submitted_at":"1993-03-18T23:27:04Z","abstract_excerpt":"We study the 3d effective field theory of a weakly coupled two Higgs-doublet scalar model at high temperature. Our model has three scalar quartic couplings and an $O(4)$ symmetry which is spontaneously broken by a nonzero scalar field $vev$ at zero temperature. Using high temperature perturbation theory, renormalization group arguments in $4-\\epsilon$ dimensions, as well as $1/N$ expansion techniques in 3 dimensions, we argue that the transition from the high temperature symmetry restoring phase to the low temperature phase is first order for a range of scalar couplings. This result is not due"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9303282","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9303282","created_at":"2026-05-18T04:37:55.501430+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9303282v2","created_at":"2026-05-18T04:37:55.501430+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9303282","created_at":"2026-05-18T04:37:55.501430+00:00"},{"alias_kind":"pith_short_12","alias_value":"UK52663MQH6D","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"UK52663MQH6DLNDC","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"UK52663M","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5","json":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5.json","graph_json":"https://pith.science/api/pith-number/UK52663MQH6DLNDCTK65RDVQV5/graph.json","events_json":"https://pith.science/api/pith-number/UK52663MQH6DLNDCTK65RDVQV5/events.json","paper":"https://pith.science/paper/UK52663M"},"agent_actions":{"view_html":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5","download_json":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5.json","view_paper":"https://pith.science/paper/UK52663M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9303282&json=true","fetch_graph":"https://pith.science/api/pith-number/UK52663MQH6DLNDCTK65RDVQV5/graph.json","fetch_events":"https://pith.science/api/pith-number/UK52663MQH6DLNDCTK65RDVQV5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5/action/storage_attestation","attest_author":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5/action/author_attestation","sign_citation":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5/action/citation_signature","submit_replication":"https://pith.science/pith/UK52663MQH6DLNDCTK65RDVQV5/action/replication_record"}},"created_at":"2026-05-18T04:37:55.501430+00:00","updated_at":"2026-05-18T04:37:55.501430+00:00"}